Method of making photoelectric conversion device

ABSTRACT

A photoelectric conversion device in which a plurality n (n being an integer larger than one) of semiconductor elements U 1  to U n  are sequentially formed on a substrate in a side-by-side relation and connected in series one after another. The substrate is formed by an insulating sheet-like member having an insulating film formed on a flexible metallic sheet-like member. The element U i  (i=1, 2, . . . n) has a first electrode E i , a non-single-crystal semiconductor laminate member Q i  formed on the first electrode E i  and having formed therein at least one PN or PIN junction, and a second electrode F i  formed on the semiconductor laminate member Q i . The element U i  is formed by the following process: (a) a first conductive layer which will ultimately serve as the first electrode E i  is formed on the substrate and then subjected to a first laser beam scanning, (b) a non-single-crystal semiconductor laminate member which will ultimately serve as the semiconductor laminate member Q i  is formed to cover the first electrode E i  and then subjected to a second laser beam scanning, (c) a second conductive layer which will ultimately serve as a second electrode F i  is formed on the semiconductor laminate member Q i  and then subjected to a third laser beam scanning.

This is a divisional application of Ser. No. 605,663, filed Apr. 30, 1984.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to improvement in or relating to a photoelectric conversion device in which a number of semiconductor elements are sequentially arranged on a substrate in side-by-side relation and connected in series.

The invention also pertains to a method for the manufacture of such a photoelectric conversion device.

2. Description of the Prior Art

A wide variety of photoelectric conversion devices have been proposed which are of the type wherein a number of semiconductor elements are formed side by side on a substrate in a sequential order.

Some of the conventional photoelectric conversion devices employ a plate-like member of glass or ceramics as the substrate; in this case, since the substrate is brittle, much care is necessary in handling the photoelectric conversion devices. Moreover, since the glass or ceramic substrate is inflexible, difficulty is encountered in mounting the photoelectric conversion device on a light receiving panel.

Sometimes the substrate is formed by a plate-like member of synthetic resin or metal; such a substrate is not readily broken and can be made flexible by reducing its thickness.

However, a substrate made of a thin plate-like member of synthetic resin, when pulled, tends to elongate as compared with a substrate formed by a thin plate-like member of metal. This introduces the possibility that elongation of the substrate caused, for example, when mounting the photoelectric conversion device on a light receiving panel, imposes a mechanical strain on the semiconductor elements sufficient to deteriorate their characteristics or break them down, making it impossible for the photoelectric conversion device to attain its required photoelectric conversion efficiency or perform its normal operation.

The substrate of synthetic resin is apt to be degenerated by light which impinges it during irradiation of the photoelectric conversion device. The degeneration of the substrate resulting from long-time service of the photoelectric conversion device often distorts the substrate itself or makes it pervious to air or water. The distortion of the substrate imposes a mechanical strain on the semiconductor elements formed thereon, resulting in degradation of their characteristics, as mentioned above. When the substrate becomes pervious to air or water, water or undesirable components pass through the substrate to reach the semiconductor elements to adversely affect them.

Accordingly, the photoelectric conversion device using a substrate of synthetic resin, when used for a long period of time, may become unable to provide the required photoelectric conversion efficiency or to stand further use.

Furthermore, the substrate of synthetic resin is readily degenerated by heat applied from the outside or generated in the semiconductor elements while in use. This also distorts the substrate or makes it pervious to air or water, cutting down the photoelectric conversion efficiency of the device or putting it out of order.

Besides, the substrate of synthetic resin is lower in heat resistance than the metallic substrate, and hence it is likely to be degenerated or deformed by heat applied for forming the semiconductor elements on the substrate. Accordingly, the use of the substrate of synthetic resin introduces difficulty in the manufacture of the photoelectric conversion device.

When the substrate is formed by a thin plate-like member of metal, there are no such defects as mentioned above. In this case, however, since the substrate surface is conductive, a relatively thick insulating layer must be interposed between the substrate and the semiconductor elements. This impairs the flexibility of the photoelectric conversion device and calls for additional steps of forming the insulating layer on the substrate prior to the formation thereon of the semiconductor elements, thus introducing complexity in the fabrication of the device by that.

There are times when the semiconductor elements on the substrate are each formed of a single-crystal semiconductor laminate member. In such a case, even slight bending of the photoelectric conversion device may impose a strain on the single-crystal semiconductor laminate member to degrade the characteristics of the semiconductor elements, resulting in the photoelectric conversion device becoming poor in its characteristics or being put out of order.

In addition, since the single-crystal semiconductor laminate member is difficult to form at low cost and with ease, its use is not preferable for the fabrication of the photoelectric conversion device.

In some of the conventional photoelectric conversion devices, the semiconductor photo elements are electrically connected in series one after another. In this case, the semiconductor elements are usually connected through the use of electrical connecting means formed by conductive layers or leads provided separately of their electrodes. But the electrical connecting means occupy a significantly large area of the substrate relative to the area occupied by the semiconductor elements on the substrate. In other words, the number of semiconductor elements formed on the substrate per unit area is small and, consequently, the photovoltage per unit area of the substrate is low. Furthermore, the electrical connecting means is required, thus introducing complexity in the manufacture of the photoelectric conversion device.

In the fabrication of the photoelectric conversion device, the semiconductor elements are usually formed by a method including the following steps (a) to (c):

(a) A first conductive layer which will ultimately act as a first electrode of each semiconductor element is formed on the substrate, a first mask of a predetermined pattern is formed (by an ordinary printing method) on the first conductive layer and then the first conductive layer is selectively etched away through the first mask, thereby providing the first electrode of each semiconductor element.

(b) A semiconductor laminate member which will ultimately serve as a semiconductor laminate member of each semiconductor element having formed thereon a PN or PIN junction is formed on the substrate in such a manner that the first electrodes of the semiconductor elements, formed by the step (a), may be buried in the semiconductor laminate member, a second mask of a predetermined pattern is formed on the semiconductor laminate member and then the semiconductor laminate member is selectively etched away through the second mask, thereby providing the semiconductor laminate member of each semiconductor element.

(c) A second conductive layer which will ultimately serve as a second electrode of each semiconductor element is formed on the substrate in such a manner that the semiconductor laminate members of the semiconductor elements, formed by the second step (b), may be buried in the second condutive layers, a third mask of a predetermined pattern is formed on the second conductive layer and then the second conductive layer is selectively etched away through the third mask, thereby providing the second electrode of each semiconductor element.

According to the conventional method including the abovesaid steps (a) to (c), the formation of the many semiconductor elements calls for three etching steps using masks, i.e. the first electrode forming step including the formation of the first mask and the selective etching through using the first mask, the semiconductor laminate member forming step including the formation of the second mask and the selective etching through using the second mask and the second electrode forming step including the formation of the third mask and the selective etching using the third mask. Accordingly, the prior art method has the defect of involving many steps for the manufacture of the photoelectric conversion device.

According to the conventional manufacturing method, the etching masks must be formed accurately in position but the positioning is very difficult, which is a serious obstacle to the fabrication of the photoelectric conversion device.

Furthermore, there is a certain limit to forming the etching masks in predetermined patterns with high precision. This imposes severe limitations on the number of semiconductor elements per unit area of the substrate and consequently the photovoltage per unit area of the substrate.

Moreover, according to the prior art manufacturing method, the semiconductor elements are usually electrically connected in series through the use of electrical connecting means formed by conductive layers or leads provided separately of the first and second electrodes of the semiconductor elements. This also constitutes an obstacle to simplification of the manufacture of the photoelectric conversion device. In addition, the electrically connecting means occupies a significantly large area of the substrate relative to the area occupied by the semiconductor elements. This also imposes severe limitations on the number of semiconductor elements per unit area of the substrate and consequently the photovoltage per unit area of the substrate.

SUMMARY OF THE INVENTION

It is therefore an object of the present invention to provide a novel photoelectric conversion device which is free from the abovesaid defects of the prior art.

Another object of the present invention is to provide a method for the manufacture of the abovesaid photoelectric conversion device.

According to the present invention, the substrate on which a number of semiconductor elements is formed side by side in succession is a insulating sheet-like member having an insulating film formed on a metallic sheet-like member. The substrate is formed by the metallic sheet-like member, and hence is not brittle, allowing ease in handling the photoelectric conversion device. And since the substrate may be flexible, the photoelectric conversion device can easily be mounted on a light receiving panel.

Moreover, the substrate is formed by the metallic sheet-like member, so that even when pulled, it hardly elongates unlike a substrate of synthetic resin. Therefore, even if the substrate is pulled, for instance, when the photoelectric conversion device is mounted on the light receiving panel, no mechanical strain is imposed on the semiconductor elements formed on the substrate. Accordingly, there is no possibility that elongation of the substrate incurs deterioration of the characteristics of the semiconductor elements and consequently the characteristics of the photoelectric conversion device.

Further, the metallic sheet-like member forming the substrate is hardly degenerated by light while in use. This assures that even long-time use of the photoelectric conversion device would not distort the metallic sheet-like member or make it pervious to air or water. On the other hand, even if the insulating film formed on the surface of the metallic sheet-like member is degenerated and distorted by light, the amount of distortion is negligibly small since the insulating film is very thin. Accordingly, even if the substrate is distorted by light, the amount of distortion is negligibly small. Besides, even if the insulating film becomes pervious to air or water, the substrate has substantially no permeability to air or water since it is formed by the metallic sheet-like member. That is to say, the substrate effectively protects the semiconductor element from water or undesirable components to maintain the characteristics of the semiconductor elements unchanged, ensuring obtainment of the required photoelectric conversion efficiency.

Moreover, the metallic sheet-like member forming the substrate is hardly degenerated by external heat or heat generated in the semiconductor elements while in use. Therefore, the metallic sheet-like member is not distorted nor does it become pervious to air or water. On the other hand, even if the insulating film formed on the metallic sheet-like member is degenerated and distorted by heat, the amount of distortion is negligibly small since the film is very thin. Accordingly, even if the substrate is distorted by heat, the amount of distortion is also negligibly small. Besides, even if the insulating film is pervious to air or water, the substrate is substantially free from permeability to air or water since it is formed by the metallic sheet-like member. Consequently, water or undesirable components from the outside do not reach the semiconductor elements through the substrate, so that the semiconductor elements are free from deterioration of their characteristics, providing required photoelectric conversion efficiency.

Furthermore, the substrate has a metallic sheet-like member and the metal material forming the metallic sheet-like member is higher in heat resistance than synthetic resin. Therefore, the metallic sheet-like member is not substantially degenerated or deformed by heat applied for the formation of the semiconductor elements on the substrate. On the other hand, even if the insulating film on the surface of the metallic sheet-like member is degenerated or deformed by heat, the amount of degeneration or deformation is negligibly small since the insulating film is very thin. Accordingly, the photoelectric conversion device of the present invention is easy to manufacture.

Moreover, since the substrate is formed by an insulating sheet-like member having the insulating film on a metallic sheet-like member, there is no need of forming a relatively thick insulating layer on the substrate prior to the formation of the semiconductor elements. This permits simplification of the manufacturing process of the photoelectric conversion device. The substrate has the insulating film formed on the surface of the metallic sheet-like member but may be highly flexible to the same extent as the flexible metallic sheet-like member because the insulating film is small in thickness. Accordingly, the photoelectric conversion device may be flexible.

Besides, in the photoelectric conversion device of the present invention in which a number of semiconductor elements are formed side by side on the substrate, the substrate is formed by the aforementioned insulating sheet-like member, and the semiconductor elements are each formed by a non-single-crystal semiconductor laminate member.

In the case of such a photoelectric conversion device of the present invention, even if bending of the device imposes a strain on the non-single-crystal semiconductor laminate member forming the semiconductor element, the characteristics of the semiconductor element are not substantially degraded and, consequently, there is no likelihood that the photoelectric conversion device will not attain the required characteristics. Since the non-single-crystal semiconductor laminate member can be obtained at low cost and with ease as compared with the single-crystal semiconductor laminate member, the photoelectric conversion device can be fabricated at lower cost and with more ease than in the case where the semiconductor elements are each formed by the single-crystal semiconductor laminate member.

In addition, according to the present invention, the semiconductor elements formed on the substrate are electrically connected in series with one another through electrical connecting means so that a second electrode of one of adjacent semiconductor elements is coupled with a first electrode of the other semiconductor element via a coupling portion formed by an extension of the second electrode of the first-mentioned semiconductor element.

With such an arrangement, the area of the substrate occupied by the electrically connecting means relative to the area occupied by the semiconductor elements is smaller than in the case where conductive layers or leads are provided seperately of the first and second electrodes of adjacent electrodes for interconnecting them. This makes it possible to increase the number of semiconductor elements per unit area as compared with the case of using the conductive layers or leads provided separately of the first and second electrodes of adjacent semiconductor elements. Consequently, the photovoltage per unit area of the substrate can be raised.

Furthermore, according to the present invention, the electrical connecting means can be formed simultaneously with the formation of the second electrodes of the semiconductor elements, namely, no particular step is needed for forming the electrical connecting means.

According to the manufacturing method of the present invention, the semiconductor elements are formed by a process including the following steps (a) to (c):

(a) A first conductive layer which will ultimately serve as a first electrode of a plurality of semiconductor elements is formed on the substrate and the first conductive layer is subjected to first scanning by a laser beam, thereby providing the first electrode of each semiconductor element.

(b) A non-single-crystal semiconductor laminate member which will ultimately serve as a non-single crystal semiconductor laminate member of each semiconductor element having formed therein a PN or PIN junction is formed on the substrate in such a manner as to cover the first electrodes of the semiconductor elements, formed by the step (a), and the non-single-crystal semiconductor layer is subjected to a second scanning by a laser beam, thereby providing the non-single-crystal semiconductor laminate member of each semiconductor element.

(c) A second conductive layer which will ultimately serve as a second electrode of each semiconductor element is formed on the substrate in such a manner as to cover the non-single-crystal semiconductor laminate members of the semiconductor elements, formed by the step (b), and the subjected to a third scanning by a laser beam, thereby providing the second electrode of each semiconductor element.

According to the manufacturing method of the present invention including the abovesaid steps (a)-(c), since the semiconductor elements can be formed by use of a scanning laser beam, the photoelectric conversion device can be fabricated with more ease and with less steps than in the case of the conventional method including etching steps using masks.

Further, according to the manufacturing method of the present invention, since the laser beam scanning can be carried out accurately in position under the control or a computer, the semiconductor elements can be formed in a predetermined pattern with high precesion. This allows more ease in the manufacture of the photoelectric conversion device than in the case of employing the conventional method including the etching steps. Moreover, the number of semiconductor elements per unit area of the substrate and consequently the photovoltage per unit area of the substrate can easily be increased.

Besides, according to the manufacturing method of the present invention, the semiconductor elements are electrically connected at the same time as their second electrodes are formed. Accordingly, the photoelectric conversion device can more easily be manufactured than in the case of using the conventional method according to which the first and second electrodes of the semiconductor elements are connected by the electrical connecting means formed by conductive layers or leads provided separately of the electrodes. In addition, according to the present invention, the area of the substrate occupied by the semiconductor elements is smaller than in the case of the conventional method using the abovesaid electrical connecting means, the number of semiconductor elements per unit area of the substrate is larger than that obtainable with the conventional method. Consequently, the photoelectric conversion device with higher photovoltage than that obtainable with the conventional method can be easily manufactured.

Further, according to the manufacturing method of the present invention, the first conductive layer formed on the substrate is subjected to a first scanning by the laser beam in the abovesaid first step (a). In this case, the substrate is an insulating sheet-like member having an insulating film on a metallic sheet-like member, as described previously in connection with the semiconductor photoelectric conversion device of the present invention. The insulating film of the substrate can be formed of an organic resin of a sufficiently low thermal conductivity. The use of such an organic resin for the insulating film of the substrate prevents heat generated in the first conductive layer by the first laser beam scanning thereof from unnecessarily escaping to the outside through the substrate. This ensures effective accomplishment of the first laser beam scanning of the first conductive layer. Accordingly, the first electrodes of the semiconductor elements can easily be formed into desired patterns with high accuracy.

Other objects, features and advantages of the present invention will become more fully apparent from the following detailed description taken in conjunction with the accompanying drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a plan view schematically illustrating an embodiment of the present invention;

FIG. 2 is a schematic sectional view taken on the line II--II in FIG. 1;

FIG. 3 is a detailed cross-sectional view showing on an enlarged scale parts of the embodiment of the present invention shown in FIG. 2;

FIGS. 4A to 4G are cross-sectional views schematically showing a sequence of steps involved in the manufacture of the photoelectric conversion device of the embodiment of the present invention depicted in FIGS. 1 to 3;

FIGS. 5 to 12 are schematic cross-sectional views, similar to FIG. 3, illustrating other embodiments of the present invention, respectively;

FIG. 13 is a plan view schematically illustrating another embodiment of the present invention;

FIG. 14 is a schematic cross-sectional view taken on the line XIV--XIV in FIG. 13; and

FIGS. 15A to 15H are a schematic cross-sectional views showing a sequence of steps involved in the manufacture of the photoelectric conversion device depicted in FIGS. 13 and 14.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

A description will be given first, with reference to FIGS. 1 to 3, of an embodiment of the present invention.

The embodiment of the photoelectric conversion device of the present invention shown in FIGS. 1 to 3 has a plurality n (n being an integer larger than one) of semiconductor photoelectric conversion elements U₁ to U_(n) formed side by side on a substrate 1.

The substrate 1 is formed by a flexible, insulating sheet-like member having an insulating film 3 formed on the surface of a flexible metallic sheet 2. The substrate 1 is, for example, rectangular in shape and 20 cm wide and 60 cm long.

The flexible metallic sheet-like member 2 forming the substrate 1 is made, for instance, of aluminum, an aluminum-base alloy or stainless steel and has a thickness of, for example, 10 to 200 μm, preferably, 50 to 150 μm.

The insulating film 3 formed on the surface of the flexible metallic sheet-like member 2 may be, for example, an oxide film resulting from oxidation of the surface of the sheet-like member. When the flexible metallic sheet-like member 2 is made of aluminum or an aluminum-base alloy, the abovesaid oxide film is an aluminum oxide (alumina Al₂ O₃) or an insulating material consisting principally of aluminum oxide. The oxide film has a thickness small enough not to impair the flexibility of the flexible metallic sheet-like member 2, for instance, in the range of 0.1 to 2 μm, preferably, 0.3 to 1 μm. Such an oxide film can be formed by heating the flexible metallic sheet-like member 2 made of aluminum or aluminum-base alloy.

The insulating film 3 may be the abovesaid oxide film but, preferably, is a film of a material whose thermal conductivity is sufficiently lower than that of an inorganic insulating material, for example, glass (having a thermal conductivity of 2×10⁻³ cal/sec/cm/°C. and a melting point of 500° to 600° C.). As such a film there can be used a film of an organic resinous material such as polyethylene terephthalate (PET) resin (thermal conductivity 6.9×10⁻⁴ cal/sec/cm/°C., melting point 260° C.), polyimide resin (thermal conductivity 4.3×10⁻⁴ cal/sec/cm/°C.), polyether sulfone (PES) resin (4×10⁻⁴ cal/sec/cm/°C.) or polyether ether ketone (PEEK) resin (thermal conductivity 6×10⁻⁴ cal/sec/cm/°C., melting point 334° C.), preferably, polyimide resin. The insulating film 3 of such an organic resin is 0.1 to 5 μm thick and can be formed by coating and drying.

The semiconductor photoelectric conversion element U_(i) (i=1, 2, . . . n) on the substrate 1 has an electrode E_(i) formed on the substrate 1, a non-single-crystal semiconductor laminate member Q_(i) formed on the electrode E_(i) and an electrode F_(i) formed on the non-single-crystal semiconductor laminate member Q_(i) in opposing relation to the electrode E_(i).

The electrode E_(i) is, for example, rectangular in shape and has a width of 5 to 40 mm, preferably 15 mm and a length slightly smaller than the length of the substrate 1.

Electrodes E_(j) (j=1, 2, . . . (n-1)) and E_(j+1) are spaced apart by a groove G_(j) which is shown to extend in the vertical direction in FIG. 1. The groove G_(j) is, for example, 40 μm wide.

The electrode E_(i) may be a non-reflective electrode but may be a reflective one.

When the electrode E_(i) is a reflective electrode, light incident on the non-single-crystal semiconductor laminate member Q_(i) on the opposite side from the substrate 1 passes through the non-single-crystal semiconductor laminate member Q_(i), then is reflected by the surface of the electrode E_(i) back to the non-single-crystal semiconductor laminate member Q_(i) to pass therethrough. The larger the optical path length of the reflected light in the non-single-crystal semiconductor laminate member Q_(i) is, the more the utilization efficiency of light is raised. From this point of view, it is preferable that the surface of the electrode E_(i) on the side of the non-single-crystal semiconductor laminate member Q_(i) have irregularities oblique to planes perpendicular to the substrate surface to form a diffuse reflection surface 6 at the boundary between it and the non-single-crystal semiconductor laminate member Q_(i) as shown in FIG. 3.

In the case where the electrode E_(i) is reflective, it may be of a single layer structure formed by a reflective conductive layer.

In order to simultaneously satisfy the requirements that the electrode E_(i) be of high conductivity and high reflectivity and to prevent that when the non-single-crystal semiconductor laminate member Q_(i) is formed, the material of its non-single-crystal semiconductor layer on the side of the electrode E_(i) or an impurity contained therein reacts with the material of the reflective electrode to form a layer of high contact resistance in the interface between the electrode E_(i) and the non-single-crystal semiconductor layer Q_(i), it is preferable that the reflective electrode E_(i) be of two-layer structure composed of a reflective conductive layer 4 and a light transparent conductive layer 5 formed on the layer 4 as shown in FIG. 3.

In the case where the electrode E_(i) is such a reflective electrode of the two-layer structure made up of the reflective conductive layer 4 and the light transparent conductive layer 5, the reflective conductive layer 4 may preferably by made of metal. The metal may be stainless steel but, in view of the requirements of high conductivity and high reflectivity for the electrode E_(i), it is preferable to employ aluminum (Al), silver (Ag), an aluminum-base alloy containing, for example, 0.1 to 2 volume % of silicon, or a silver-base alloy.

The light transparent conductive layer 5 may preferably be made of a metal oxide. In this case, in order to ensure that the layer 5 be high in conductivity and in transmittance and to prevent that when the non-single-crystal semiconductor laminate layer Q_(i) is formed, reaction of the metallic oxide with the material or impurity of the non-single-crystal semiconductor layer of the laminate member Q_(i) on the side of the electrode E_(i) to form the abovesaid high contact resistance layer, it is preferable to form the layer 5 of a tin oxide (SnO₂ or SnO) or a metallic oxide consisting principally of such a tin oxide, for instance, a tin oxide containing halogen or, 1 to 10 wt % of antimony oxide in the event that the non-single-crystal semiconductor layer of the non-single-crystal semiconductor laminate member Q_(i) on the side of the electrode E_(i) is p-type. In the case where the layer of the non-single-crystal semiconductor laminate member Q_(i) on the side of the electrode E_(i) is N-type, it is preferable to use an indium oxide or a metallic oxide consisting principally thereof, for instance, an indium oxide containing 1 to 10 wt % of tin oxide. In this case, the light transparent conductive layer 5 is 300 to 600 Å thick.

In the case where the electrode E_(i) is such a two-layer reflective electrode comprising the layer 4 and the layer 5, when the abovesaid diffuse reflection surface 6 is formed at the boundary between the electrode E_(i) and the non-single-crystal semiconductor laminate member Q_(i), it is formed on the surface of the layer 5 on the side of the laminate member Q_(i).

In the semiconductor element U_(i) formed on the substrate 1, the non-single-crystal semiconductor laminate member Q_(j+1) (j=1, 2, . . . (n-1)) on the aforesaid electrode E_(j+1) extends laterally from the marginal edge of the electrode E_(j+1) on the opposite side from the electrode E_(j) to a position on the electrode E_(j) on the side of the electrode E_(j+1) across the groove G_(j) separating the electrode E_(j) and E_(j+1) making contact with the non-single-crystal semiconductor laminate member Q_(j).

The non-single-crystal semiconductor laminate member Q₁ formed on the electrode E₁ extends laterally onto the substrate 1 to cover the side surface of the electrode E₁ on the opposite side from the electrode E₂.

Further, the non-single-crystal semiconductor laminate member Q_(n) is formed as a non-single-crystal-semiconductor laminate member Q₀ to laterally extend onto the substrate 1 to cover the side surface of the electrode E_(n) on the opposite side from the electrode E_(n-1).

The non-single-crystal semiconductor laminate member Q_(i) is formed to vertically extend to cover the electrode E_(i). The non-single-crystal semiconductor laminate member Q_(i) has cut therein a groove O_(i). The groove O_(i) may be extended across the entire width of the semiconductor laminate member Q_(i), as shown in FIG. 1, but it may also be extended to the vicinity of either side of the semiconductor laminate member Q_(i) thereacross. Also it is possible to cut the groove O_(i) in a discontinuous form lengthwise of the semiconductor laminate member Q_(i). The grooves O₁ to O_(n) are formed simultaneously.

The non-single-crystal semiconductor laminate member Q_(i) formed on the electrode E_(i) may be formed by one or more two-layer structures, each composed of a P-type or N-type non-single-crystal semiconductor layer and another non-single crystal semiconductor layer of the opposite conductivity type. Accordingly, the non-single-crystal semiconductor laminate member Q_(i) can be formed to have at least one PN junction.

Furthermore, the non-single-crystal semiconductor laminate member Q_(i) may preferably be formed by one or more three-layer structures, each composed of a P-type or N-type non-single-crystal semiconductor layer 8, an I-type non-single-crystal semiconductor layer 9 and a non-single-crystal semiconductor layer 10 opposite in conductivity type to the layer 8, as shown in FIG. 3. Accordingly, the non-single-crystal semiconductor laminate member Q_(i) may preferably be formed to have at least one PIN junction.

The non-single-crystal semiconductor layer of the non-single-crystal semiconductor laminate member Q_(i) on the side of the electrode E_(i) is P-type when the electrode E_(i) is made up of the reflective conductive layer 4 and the light transparent conductive layer 5 as described above and as illustrated in FIG. 3 and the light transparent conductive layer 5 is formed by a tin oxide or metallic oxide consisting principally of the tin oxide as described previously with respect to FIG. 3. When the layer 5 of the electrode E_(i) making contact with the non-single-crystal semiconductor laminate member Q_(i) is formed by an indium oxide or metallic oxide consisting principally of indium oxide, the non-single-crystal semiconductor layer of the non-single-crystal semiconductor laminate member Q_(i) on the side of the electrode E_(i) is N-type.

Accordingly, in the case where the non-single-crystal semiconductor laminate member Q_(i) has the three-layer structure comprising the non-single-crystal semiconductor layers 8, 9 and 10 as illustrated in FIG. 3 and the electrode E_(i) comprises the reflective conductive layer 4 and the light transparent conductive layer 5 and the light conductive layer 5 is formed by tin oxide or metallic oxide consisting principally of tin oxide, the non-single-crystal semiconductor layers 8 and 10 are P-type and N-type, respectively. When the light transparent conductive layer 5 is formed by indium oxide or metal oxide consisting principally of indium oxide, the non-single-crystal semiconductor layers 8 and 10 are N-type and P-type, respectively.

The non-single-crystal semiconductor layers making up the non-single-crystal semiconductor laminate member Q_(i) may preferably be formed of silicon or a semiconductor consisting principally of silicon but it may also be formed of other semiconductors.

When the non-single-crystal semiconductor laminate member Q_(i) has the three-layer structure composed of the non-single-crystal semiconductor layers 8, 9, and 10, the non-single-crystal semiconductor layer 8 may be formed, for instance, of silicon to a thickness of 5 to 300 Å, preferably 70 to 130 Å. Where the non-single-crystal semiconductor layer 8 is P-type, for example, boron (B) may be introduced thereinto as a P-type impurity.

The non-single-crystal semiconductor layer 9 can be formed of silicon as is the case with the non-single-crystal semiconductor layer 8 but its thickness may preferably be larger than that of the layer 8, for instance, 0.4 to 0.7 μm. The non-single-crystal semiconductor layer 9 contains a very small amount of a P-type impurity or does not substantially contain either of P-type and N-type impurities and, if any, their concentrations are negligibly low.

The non-single-crystal semiconductor layer 10 can also be formed of silicon as is the case with the non-single-crystal semiconductor layer 8. But since the non-single-crystal semiconductor layer 10 is disposed on the wide where the light to be converted is incident on the semiconductor element, it may preferably be formed of a semiconductor which has a larger energy band gap than does the semiconductor material of the non-single-crystal semiconductor layer 8, such as, for example, silicon carbide, expressed by Si_(x) C_(1-x) (0<x<1). In this case, the non-single-crystal semiconductor layer 10 can be formed to a thickness of 5 to 300 Å, typically, in the range of 7 to 130 Å.

Incidentally, the aforesaid non-single-crystal semiconductor laminate member Q₀ has the same structure as the aforementioned member Q_(i).

In the semiconductor element U_(i) formed on the substrate 1, the electrode F_(i) on the non-single-crystal semiconductor laminate member Q_(i) is disposed opposite to the electrode E_(i) formed on the non-single-crystal semiconductor laminate member Q_(i).

In this case, the electrode F_(j+1) extends from a position apart from the portion 13 of the non-single-crystal semiconductor laminate member Q_(j+1) on the opposite side from the non-single-crystal semiconductor laminate member Q_(j) onto its portion 13 on the side of the non-single-crystal semiconductor laminate member Q_(j+1).

The electrode F₁ extends from a position away from the end portion of the non-single-crystal laminate member Q₁ on the side of the non-single-crystal semiconductor laminate member Q₂ to the marginal edge of the substrate 1 to cover the extension of the non-single-crystal laminate member Q₁ on the side surface of the electrode E₁.

On the non-single-crystal semiconductor laminate member Q_(n), an electrode F₀ similar to the electrode F_(n) is formed to extend from the portion 13 on the side of the non-single-crystal semiconductor laminate member Q₀ to the marginal edge of the substrate 1 to cover the side surface of the non-single-crystal semiconductor laminate member Q₀.

The electrodes F_(j) and F_(j+1) are isolated by an isolating portion H_(j). The electrodes F_(j+1) and F₀ are also isolated by an isolating portion H_(n). The isolating portions H_(i) may be simultaneously formed as grooves as is the case with the grooves G_(i).

The electrode F_(i) may be formed as a single layer structure as shown in FIG. 3 and may also be of the two-layer structure. Also it is possible to employ a three-layer structure.

The electrode F_(i) is a transparent conductive layer and formed, for example, of a metallic oxide. In this case, it is required that the metal oxide be high in conductivity and in transmittance and, when forming the electrode F_(i), would not react with the material or impurity of the non-single-crystal semiconductor layer of the non-single-crystal semiconductor laminate member Q_(i) on the side of the electrode F_(i) to form a layer which increases the contact resistance between the non-single-crystal semiconductor laminate member Q_(i) and the electrode F_(i) or a layer of low transmittance. To meet such requirements, when the non-single-crystal layer of the non-single-crystal semiconductor laminate member Q_(i) on the side of the electrode F_(i) is N-type, the electrode F_(i) may preferably be formed of an indium oxide or metallic oxide consisting principally of indium oxide, such as, for example, an indium oxide contaning 1 to 10 wt % of tin oxide. When the non-single-crystal layer of the non-single-crystal semiconductor laminate member Q_(i) on the side of the electrode F_(i) is P-type, the electrode F_(i) may preferably be formed of a tin oxide or metallic oxide consisting principally of tin oxide. The electrode F_(i) can be formed, for instance, 300 to 600 Å thick.

In the case where the electrode Fi has the two-layer structure, the layer making contact with the non-single-crystal semiconductor laminate member Q_(i) may preferably be a layer formed of tin oxide or consisting principally thereof, or a layer formed of the indium oxide or consisting principally thereof as described previously depending on whether the non-single-crystal semiconductor layer of the non-single-crystal semiconductor laminate member Q_(i) is P-type or N-type. In this case, it is preferable that when the layer making contact with the non-single-crystal semiconductor laminate member Q_(i) is formed of tin oxide or consisting principally thereof, the other layer be a layer formed of indium oxide or consisting principally thereof and, when the layer making contact with the laminate member Q_(i) is formed of the indium oxide or consisting principally thereof, the other layer be a layer formed of tin oxide or consisting principally thereof.

The electrode F₀ formed to extend on the non-single-crystal semiconductor laminate member Q₀ has the same structure as the abovesaid electrode F_(i).

The electrode F_(j+1) of the semiconductor element U_(j+1) (j=1, 2, . . . (n-1)) is coupled with the electrode E_(j) of the semiconductor element U_(j) through a coupling portion K_(j).

The coupling portion K_(j) extends from the position where the electrode F_(j+1) is opposite to the electrode E_(j) to the region of the electrode E_(j+1) opposite to the electrode F_(j+1), passing through a groove O_(j) by which the non-single-crystal semiconductor laminate members Q_(j) and Q_(j+1) are separated. Such a coupling portion K_(j) is formed by an extension of the electrode F_(j+1) formed simultaneously with the electrode F_(j+1).

The electrode F₁ of the semiconductor element U₁ extends down to the surface of the substrate 1 as referred to previously and the extension constitutes an external connection terminal 11.

The electrode F₀ extending on the non-single-crystal semiconductor laminate member Q₀ is coupled with the electrode E_(n) of the semiconductor element U_(n) through a coupling portion K_(n). In this case, the coupling portion K_(n) extends from the position where the electrode F₀ is opposite to the electrode E_(n) to the region 14 of the electrode E_(n) opposite to the electrode F₀, passing through a groove O_(n). Such a coupling portion K_(n) is an extension of the electrode F₀ formed simultaneously therewith. The electrode F₀ extends on the side surface of the non-single-crystal semiconductor laminate member Q₀ in the direction away from the electrode F_(n) to the marginal edge of the substrate 1, and the extending end portion forms a terminal 12 for external connection.

The isolating portion H_(j) is formed to extend in the vertical direction in FIG. 1 to go down into the non-single-crystal semiconductor laminate member Q_(j) to form therein a region 13 underlying the electrode F_(j+1). The groove O_(j) also extends across that portion of the electrode E_(j) adjacent to the electrode E_(j+1) in the thickwise direction. Accordingly, the electrode E_(j) has an isolating portion 14 on the side of the electrode E_(j+1).

The isolating portion H_(n) is formed to extend in the vertical direction in FIG. 1 to go down into the non-single-crystal semiconductor laminate member Q_(n) to form therein the region 13 underlying the electrode F₀.

The groove O_(n) extends across that portion of the electrode E_(n) on the opposite side from the electrode F₀ in the thickwise direction. Accordingly, the electrode E_(n) has the isolated region 14 on the opposite side from the electrode E_(n-1).

A transparent antireflection and protective film 15 is formed on the upper surface of the array to cover the aforesaid semiconductor elements U₁ to U_(n). In this case, however, the antireflection and protective film 15 does not extend on the extended portions of the electrodes F₁ and F₀ forming the aforementioned external connection terminals 11 and 12, respectively.

The foregoing is a description of the arrangement of an embodiment of the photoelectric conversion device according to the present invention.

Next, a description will be given, with reference to FIGS. 4A to 4G, of an embodiment of the photoelectric conversion device manufacturing method of the present invention.

In FIGS. 4A to 4G, parts corresponding to those in FIGS. 1 and 2 are identified by the same reference numerals and characters and no detailed description thereof will be repeated.

The manufacturing method of the photoelectric conversion device shown in FIGS. 4A to 4G is as follows:

The manufacture starts with the preparation of a substrate 1 as shown in FIG. 4A which is formed by an insulated sheet-like member having an insulating film 3 formed on the surface of a metallic sheet-like member 2 as described previously with respect to FIGS. 1 and 2.

Then, as shown in FIG. 4B, the conductive layer 41 which will ultimately form the electrodes E₁ to E_(n) described previously in connection with FIGS. 1 and 2 is formed by known method on the substrate 1.

In the case where the electrodes E₁ to E_(n) are each formed to have the two-layer structure composed of the two layers 4 and 5 as described previously with regard to FIG. 3, the conductive layer 41 is made up of a layer which will ultimately serve as the layer 4 and another layer which ultimately serve as the layer 5, though neither are shown nor described in detail. The former layer is first formed on the substrate 1 by a known method, for example, vapor deposition, and then the latter layer is similarly formed thereon by a known method, for instance, vapor deposition.

In this case, the conductive layer for the light transparent conductive layer 5 can be formed so that its surface may cause diffuse reflection at the boundary between the electrode E_(i) and the non-single-crystal semiconductor laminate member Q_(i).

Next, the conductive layer 41 is scanned by a laser beam (not shown) having a diameter of 30 to 70 μm, typically, 40 μm, by which the aforementioned (n-1) grooves G_(i) to G_(n-1) are cut in the conductive layer 41 to form n electrodes E₁ to E_(n) which are separated from adjacent ones by grooves G₁ to G_(n-1), as shown in FIG. 4C. For this scanning, it is possible to employ a laser beam of a 1.06 μm wavelength from a YAG laser and a laser beam of a 0.488 or 0.512 μm wavelength from an argon laser.

The abovesaid laser beam scanning can be carried out in the air but may also be performed in the atmosphere of a gas or liquid which reacts with the conductive material of the layer 41 at high temperatures to spatter it from the substrate surface.

In this case, the gas used may be hydrogen fluoride (HF), hydrogen chloride (HCl), or Freon gas (CF₄, CHF₃, CClF₃ and like gases).

Liquids which can be used include hydrofluoric acid (HF), hydrochloric acid (HCl) or Freon liquid (C₂ F₃ Cl₄, C₂ F₃ Cl₃ or the like).

In the case where the laser beam scanning takes place in the air, burrs are likely to form on the upper marginal edges of the groove G_(j). Accordingly, it is desirable that the laser beam scanning be followed by deburring through the use of the abovesaid gas or etching with an etchant such as hydrofluoric acid (HF), hydrochloric acid (HCl), or Freon liquids (C₂ F₃ Cl₄, C₂ F₃ Cl₃ or similar liquids).

Moreover, it is possible to accomplish the laser beam scanning of the conductive layer 41 easily and accurately by the aid of a computer while monitoring through a video camera device.

Next, a non-single-crystal semiconductor layer 42, which will ultimately form the non-single-crystal semiconductor laminate members Q₁ to Q_(n) and Q₀ described previously with respect to FIGS. 1 and 2, is formed by a known method, for example, low-pressure CVD on the substrate 1 to fill the grooves G₁ to G_(n-1) and to cover the electrodes E₁ to E_(n), as shown in FIG. 4D, so that the regions of the layer 42 on the electrodes E₁ to E_(n) may be the non-single-crystal semiconductor laminate members Q₁ to Q_(n) described previously with respect to FIGS. 1 and 2.

Where the non-single-crystal semiconductor laminate members Q₁ to Q_(n) are each formed as the three-layer structure consisting of the non-single-crystal semiconductor layers 8, 9 and 10 as described previously with regard to FIG. 3, non-single-crystal semiconductor layers which will ultimately be used as the non-single-crystal layers 8, 9 and 10 respectively, are formed in this order through the use of a known method, for instance, the low-pressure CVD method, thereby providing the non-single-crystal semiconductor laminate member 42.

After this, the non-single-crystal semiconductor laminate members Q₁ to Q_(n) are selectively removed by laser beam scanning to cut therein the aforementioned n grooves O₁ to O_(n), as shown in FIG. 4E.

In this case, the groove O_(i) (i=1, 2, . . . n) can be formed to extend down to the insulating film 2 of the substrate 1 across the electrode E_(i) as illustrated. In such a case, the region 14 of the electrode E_(i) is isolated from the other regions.

The laser beam scanning of the non-single-crystal semiconductor laminate members 42 and the electrodes E₁ to E_(n) can take place in the air, as is the case with the conductive layer 41. It is also possible to carry out the laser beam scanning in the atmosphere of a gas which reacts with the materials of the non-single-crystal semiconductor laminate member 42 and the electrodes E₁ to E_(n) at high temperatures to spatter them from the substrate surface. Also in this case, the gas used is hydrogen fluoride, hydrogen chloride, or Freon gas.

The laser beam scanning can also be carried out in a liquid which reacts with the materials of the laminate member 42 and the electrodes E₁ to E_(n) at high temperature to remove them from the substrate surface. The liquid in this case can be hydrofluoric acid, hydrochloric acid, and the Freon liquid as is the case with the conductive layer 41.

In the case where the laser beam scanning of the non-single-crystal semiconductor laminate members 42 and the electrodes E₁ to E_(n) is carried out in the air, it is desirable that the laser beam scanning be followed by deburring through the use of the aforesaid gas or etching with such etchants as mentioned previously.

The abovesaid laser beam scanning can also be performed easily and accurately with the aid of a computer while monitoring through a video camera device.

The groove O_(j) (j=1, 2, . . . (n-1)) is formed at a position spaced a predetermined distance apart from the groove G_(j) laterally thereof (on the left thereof in FIG. 5). The predetermined distance is large as compared with the thickness of the non-single-crystal semiconductor laminate member 42. It is preferable, however, to minimize this distance. By the aid of a computer the groove O_(j) can be provided in close proximity to the groove G_(j) with high accuracy. This permits reduction of the area of the substrate 1 occupied by the region 14 of the electrode E_(j). It is desirable that the groove O_(n) be formed closely to the marginal edge of the electrode E_(n) on the opposite side from the electrode E_(n-1) so that the region 14 of the electrode E_(n) may occupy less area of the substrate 1.

Next, a conductive layer 43, which will ultimately form the electrodes F₁ to F_(n) and F₀ referred to with respect to FIGS. 1 and 2, is formed, for example, by vapor deposition on the substrate 1 to cover the non-single-crystal semiconductor laminate members Q₁ to Q_(n) and to fill the grooves O₁ to O_(n), forming coupling portions K₁ to K_(n) (FIG. 4F).

In this case, the conductive layer 43 is formed to extend on the substrate 1 except for both marginal portions in its widthwise direction but it covers both marginal portions of the substrate 1 in its lengthwise direction.

Next, as shown in FIG. 4G, the conductive layer 43 is selectively removed by laser beam scanning as is the case with the non-single-crystal semiconductor laminate members 42. By this laser beam scanning there are formed in the conductive layer 43 n isolating portions H₁ to H_(n), by which n electrodes F₁ to F_(n) isolated by the isolating portions H₁ to H_(n-1), respectively, and opposite to the electrodes E₁ to E_(n) across the non-single-crystal semiconductor laminate members Q₁ to Q_(n), respectively, and an electrode F₀ isolated by the isolating portion H_(n) from the electrode F_(n) and opposite to electrode E_(n) are formed. In this case, the laser beam scanning is carried out so that the electrode F_(j+1) may be linked with the electrode E_(j) through the coupling portion K_(j) and so that the electrode F₀ may be linked with the electrode E_(n) through the coupling portion K_(n).

By the abovesaid laser beam scanning, the isolating portion H_(i) (i=1, 2, . . . n) can be formed to extend into the non-single-crystal semiconductor laminate member Q_(i).

As is the case with the conductive layer 41, the laser beam scanning of the conductive layer 43 can be effected in the air and may also be carried out in the atmosphere of a gas which reacts with the materials of the conductive layer 43 and the non-single-crystal semiconductor laminate members Q₁ to Q_(n) at high temperatures to spatter them from the substrate surface. The gas used in this case may be hydrogen fluoride, hydrogen chloride, or Freon gas. It is also possible to conduct the laser scanning in a liquid which reacts with the materials of the conductive layer 43 and the non-single-crystal semiconductor laminate members Q₁ to Q_(n) and high temperatures to remove them from the substrate surface. The liquid used in this case may be hydrofluoric acid, hydrochloric acid, or Freon liquid.

Also in the case of performing the laser beam scanning of the conductive layer 43 in the air, it is desirable that the laser beam scanning be followed by deburring through the use of the aforesaid gas or etching using the aforesaid liquid as the etchant.

By the laser beam scanning for the conductive layer 43, the isolating portion H_(i) can be provided in the form of a groove as illustrated.

The laser beam scanning of the conductive layer 43 can also be carried out easily and accurately with the aid of a computer while monitoring through a video camera device.

Further, the isolating portion H_(i) is formed a predetermined distance apart from the groove O_(i) laterally thereof (on the left thereof in the drawing). The predetermined distance is large as compared with the thickness of the non-single-crystal semiconductor laminate member 43, but it may preferably be selected as small as possible. By the aid of a computer the isolating portion H_(i) can be formed in close proximity to the groove O_(i) with high precision. This allows reduction of the area of the substrate 1 occupied by the region 13 formed in the non-single-crystal semiconductor laminate member Q_(i).

Next, a transparent antireflection and protective film 15 is formed by a known method on the array to cover the electrodes F₁ to F_(n) and F₀ and the isolating portion H₁ as shown in FIG. 4G.

In the manner described above, the photoelectric conversion device of the present invention, shown in FIGS. 1 and 2, is manufactured.

The above is a description of an embodiment of the present invention and an example of its manufacturing method.

According to the photoelectric conversion device of FIGS. 1 and 2, when light (not shown) is incident thereon from the side of the substrate 1 or the electrodes F₁ to F_(n) each semiconductor element U_(i) (i=1, 2, . . . n) carries out photoelectric conversion to generate photovoltage across its electrodes E_(i) and F_(i).

The electrodes F_(j+1) (j=1, 2, . . . (n-1)) of the semiconductor element U_(j+1) is linked with the electrode E_(j) of the semiconductor element U_(j) through the coupling portion K_(j) and the electrode F₁ of the semiconductor element U₁ is connected to an external connection terminal 11 and the electrode E_(n) of the semiconductor element U_(n) is connected to an external connection terminal 12 through the coupling portion K_(n) and the electrode F₀.

Accordingly, the semiconductor elements U₁ to U_(n) are sequentially connected in series through the coupling portions K₁ to K_(n-1) and connected to the external connection terminals 11 and 12.

Consequently, upon incidence of light, there is developed across the external connection terminals 11 and 12 the photovoltage that is equal to the sum of voltage produced by the semiconductor elements U₁ to U_(n).

According to the embodiment of FIGS. 1 and 2, since the substrate 1 is formed by an insulating sheet-like member having an insulating film 3 formed on the surface of a metallic sheet-like member 2, the photoelectric conversion device of the present invention is advantageous in that it is easy to handle and hence easy to mount on a light receiving panel, and its characteristics are not degraded when it is mounted on the light receiving panel, or by long-time service, as referred to previously. The advantages are more marked in the cases where the insulating sheet-like member is flexible.

In the embodiment of FIGS. 1 and 2 the semiconductor elements U₁ to U_(n) are formed by the non-single-crystal semiconductor laminate members Q₁ to Q_(n), respectively. Therefore, even if the substrate 1 is bent to impose a strain on the non-single-crystal semiconductor laminate members Q₁ to Q_(n) to some extent, the characteristics of the photoelectric conversion device are not degraded, and the device can easily be fabricated at low cost, as described previously.

Moreover, the semiconductor elements U₁ to U_(n) are sequentially connected in series through the coupling portions K₁ to K_(1-n) and the semiconductor elements U₁ to U_(n) are connected to external connection terminals 11 and 12, respectively, as described previously. The coupling portions K₁ to K_(n) constitute electrical connecting means for electrically connecting the semiconductor elements U₁ to U_(n) in series between the external connection terminals 11 and 12 but the coupling portions K_(j) and K_(n) are formed by the extended portions of the electrodes F_(j+1) of the semiconductor element U_(j+1) and Fo.

Consequently, as described previously, the area of the substrate 1 occupied by the electrical connecting means is smaller than the area of the substrate occupied by the semiconductor elements U₁ to U_(n), so that the photovoltage per unit area of the substrate 1 is high. Further, the electrical connecting means can easily be formed. Accordingly, the photoelectric conversion device is easy to produce. In addition, by forming the electrodes E_(i) of the semiconductor element U_(i) as reflective electrodes as described previously with respect to FIG. 3, incident light can efficiently be utilized by the semiconductor U_(i), providing for increased photo-voltage per unit area of the substrate 1.

Besides, in the case where the abovesaid reflective electrode is made up of the reflective conductive layer 4 of aluminum, silver, or an alloy consisting principally of one of them, disposed on the side of the substrate 1, and the light transparent conductive layer 5 is formed on the reflective conductive layer 4 in contact with the non-single-crystal semiconductor laminate member Q_(i) as described previously with respect to FIG. 3, an excellent ohmic contact can be made between the electrode E_(i) and the non-single-crystal semiconductor laminate member Q_(i) and high reflectivity can be obtained, so that high photovoltage can be obtained from the semiconductor element U_(i) with practically no loss and the efficiency of utilization of light can be improved. These features can be made more distinct by forming the surface of the light transparent conductive layer 5 so that a diffuse reflection surface 6 may be provided at the boundary between the electode E_(i) and the non-single-crystal semiconductor laminate member Q_(i) as referred to previously in connection with FIG. 3. The abovesaid features can be made more marked by forming the light transparent conductive layer 5 of the electrode E_(i) of a tin oxide or a metallic oxide consisting principally thereof, depending on whether the non-single-crystal semiconductor layer of the semiconductor element U_(i) on the side of the electrode E_(i) is P-type or N-type.

Further, in the case where the electrodes E_(j) and E_(j+1) of the semiconductor elements U_(j) and U_(j+1) are separated by the groove G_(j) as illustrated, the non-single-crystal semiconductor laminate member Q_(j+1) of the semiconductor element U_(j+1) is formed to extend from the electrode E_(j+1) onto the portion of the electrode E_(j) on the side of the electrode E_(j+1) across the groove G_(j), the non-single-crystal semiconductor laminate members Q_(j) and Q_(j+1) are separated by the groove O_(j) on the side of the electrode E_(j) opposite from the groove G_(j) and the coupling portion K_(j) formed by the extension of the electrode F_(j+1) is coupled with the electrode E_(j) through the groove O_(j), the semiconductor elements U₁ to U_(n) can be arranged on the substrate 1 with a high density, providing for increased photovoltage per unit area of the substrate.

Where the groove O_(j) cut in the non-single-crystal semiconductor laminate member Q_(j) is extended into the electrode E_(j) as illustrated, the coupling portion K_(j) extending from the electrode F_(j+1) makes side-contact with the electrode E_(j) and hence makes good ohmic contact therewith, thereby ensuring obtainment of large electromotive force across the external connection terminals 11 and 12 with no appreciable loss.

With such an arrangement wherein the electrodes F_(j) and F_(j+1) are isolated by the isolating portion H_(j) provided on the side of the non-single-crystal semiconductor laminate member Q_(j) opposite from the groove O_(j) formed at the position opposite to the groove G_(j), the semiconductor elements U₁ to U_(n) can be arranged on the substrate 1 with higher density, providing for further increased photovoltage per unit area of the substrate 1.

Since the isolating portion H_(j) is formed to extend into the non-single-crystal semiconductor laminate member Q_(j) as illustrated, substantially no leakage occurs through the non-single-crystal semiconductor laminate members Q_(j) between the electrode E_(j) and F_(j+1), thereby ensuring obtainment of large electromotive force across the external connection terminals 11 and 12.

In the embodiment of FIGS. 1 and 2, the non-single-crystal semiconductor laminate member Q₁ of the semiconductor element U₁ is formed on the electrode E₁ to extend onto the substrate 1 and the electrode F₁ is formed on the non-single-crystal semiconductor laminate member Q₁ to similarly extend onto the substrate 1 and the extended portion is used as the external connection terminal 11. With such an arrangement, the series array of the semiconductor elements U₁ to U_(n) can easily be connected at one end to the external connection terminal 11. This permits simplification of the construction of photoelectric conversion device as a whole.

Further, in the embodiment of FIGS. 1 and 2, the non-single-crystal semiconductor laminate member Q_(n) is formed to extend on the side surface of the electrode E_(n) towards the other edge of the substrate 1. The electrode F₀ is formed on the non-single-crystal semiconductor laminate member Q_(n) to extend on to the substrate surface and the electrode F₀ is coupled with the electrode E_(n) through the coupling portion K_(n). The extended portion of the electrode F₀ on the substrate 1 is used as the external connection terminal 12. Accordingly, the series array of the semiconductor elements U₁ to U_(n) can easily be connected at one end to the external connection terminal 12, permitting simplification of the overall structure of the photoelectric conversion device.

The manufacturing method of the present invention, shown in FIG. 4, includes the following steps for the fabrication of the photoelectric conversion device shown in FIGS. 1 and 2.

(a) The first conductive layer 41 is formed on the substrate 1 formed by insulating sheet-like member having an insulating film 3 formed on a metallic sheet-like member 2 (FIG. 4B).

(b) The first conductive layer 41 is subjected to a first laser beam scanning to form therein the first grooves G₁ to G_(n-1) to provide the first electrodes E₁ to E_(n) separated by the first grooves G₁ to G_(n-1), respectively (FIG. 4C).

(c) The non-single-crystal semiconductor laminate member 42 is formed on the substrate 1 to cover the first grooves G₁ to G_(n-1) and the electrodes E₁ to E_(n) (FIG. 4D).

(d) The non-single-crystal semiconductor laminate member 42 is subjected to a second laser beam scanning to form therein the second grooves O₁ to O_(n) to expose therethrough the first electrodes E₁ to E_(n) to the outside and to provide the n non-single-crystal semiconductor laminate members Q₁ to Q_(n) defined by the second grooves O₁ to O_(n), respectively (FIG. 4E).

(e) The second conductive layer 43 is formed on the substrate 1 to continuously extend on the non-single-crystal semiconductor laminate members Q₁ to Q_(n) and into the grooves O₁ to O_(n-1) to provide coupling portions K₁ to Kn-1 which are connected to the first electrodes E₁ to E_(n-1) through the grooves O₁ to O_(n-1), respectively (FIG. 4F).

(f) The second conductive layer 43 is subjected to a third laser beam scanning to form therein the n isolating portions H₁ to H_(n-1) to provide the n second electrodes F₁ to F_(n) which are isolated by the isolating portions H₁ to H_(n-1), respectively, and are opposite to the electrodes E₁ to E_(n) through the non-single-crystal semiconductor laminate members Q₁ to Q_(n) so that the second electrodes F₂ to F_(n) are connected to the first electrodes E₁ to E_(n-1) through the coupling portions K₁ to K_(n-1), respectively (FIG. 4G).

Accordingly, the manufacturing method of the present invention shown in FIG. 4 permits easy manufacture of the photoelectric conversion device shown in FIGS. 1 and 2.

According to the manufacturing method of the present invention shown in FIG. 4, the second groove O_(j) (j=1, 2, . . . (n-1)) can easily be formed a predetermined distance apart from the first groove G_(j) but adjacent thereto and, further, the isolating portion H_(j) can easily be formed a predetermined distance apart from the first groove G_(j) but adjacent to the groove O_(j). Accordingly, the semiconductor elements U₁ to U_(n) can be formed on the substrate 1 with high density, allowing ease in the manufacture of the photoelectric conversion device which generates high photovoltage per unit area of the substrate 1.

Further, since the second groove O_(j) can easily be formed to extend in the direction of thickness of the first electrode E_(j), the coupling portion K_(j) can easily be formed in contact with the side of the first electrode E_(j) exposed to the groove O_(j). This ensures good contact between the coupling portion K_(j) and first electrode E_(j), providing for reduced internal loss.

Moreover, by performing the first laser beam scanning of the first conductive layer 41 in the air or in the atmosphere of a gas or liquid which reacts with the conductive material of the first conductive layer 41 at high temperatures to spatter it from the surface of the substrate 1, the first grooves G₁ to G_(n-1) and the first electrodes E₁ to E_(n) can easily be formed. By performing the second laser beam scanning of the non-single-crystal semiconductor layer 42 in the air or in the atmosphere of a gas or liquid which reacts with the non-single-crystal semiconductor of the non-single-crystal semiconductor laminate member 42 to spatter it from the surface of the substrate 1, the second grooves O₁ to O_(n) and the non-single-crystal semiconductor laminate members Q₁ to Q_(n) can easily be formed. By branching the third laser beam scanning of the second conductive layer 43 in the air or in an atmosphere of oxygen, or in the atmosphere of a gas or liquid which reacts with in the conductive material of the second conductive layer 43 to spatter it from the surface of the substrate 1, the isolating portions H₁ to H_(n-1) and the second electrodes F₁ to F_(n) can easily be formed. Accordingly, the photoelectric converter having the aforesaid advantages can easily be fabricated.

Furthermore, the first conductive layer 41 formed on the substrate 1 is subjected to the first laser beam scanning in the abovesaid step (b) to cut first grooves G₁ to G_(n-1) in the first conductive layer 41, providing the first electrodes E₁ to E_(n). In this case, the substrate 1 is an insulating sheet-like member having an insulating film 3 on a metallic sheet-like member 2. The insulating film 3 of the substrate 1 can be formed of an organic resin of a sufficiently low thermal conductivity. With the insulating film 3 of such an organic resin, it is possible to prevent heat generated in the first conductive layer 41 on the insulating film 3 by the first laser beam scanning thereof from unnecessarily escaping to the outside through the substrate 1. Therefore, the first laser beam scanning of the first conductive layer 41 is effectively carried out. That is, the first grooves G₁ to G_(n-1) can easily be provided without leaving therein the material of the first conductive layer 4. Therefore, the first electrodes E₁ to E_(n) of the semiconductor elements U₁ to U_(n) can easily be formed in desired patterns with high accuracy.

In addition, since the third laser beam scanning of the second conductive layer 43 can readily be carried out so that the isolating portion H_(j) may extend into the non-single-crystal semiconductor laminate member Q_(j), the non-single-crystal semiconductor laminate members Q₁ to Q_(n) can easily be formed with substantially no leakage between the non-single-crystal semiconductor laminate members Q_(j) and Q_(j+1). Accordingly, the semiconductor elements U₁ to U_(n) of the high photovoltage can easily be obtained.

A description will be given of other embodiments of the photoelectric conversion device of the present invention.

In the embodiment of the photoelectric conversion device shown in FIGS. 1 to 3, the electrodes F_(j) and F_(j+1) of the semiconductor elements U_(j) and U_(j+1) are isolated by the isolating portion H_(j) provided in the form of a groove and the isolating portion H_(j) extends across the non-single-crystal semiconductor laminate member Q_(i).

The embodiment of FIG. 5 corresponding to FIG. 3 is identical in construction with the embodiment of FIGS. 1 to 3 except that the isolating portion H_(j) does not extend through the non-single-crystal semiconductor laminate member Q_(i).

Such isolating portions H_(j) can easily be formed by adjusting the scanning and/or power of the laser beam in the laser beam scanning of the conductive layer 43 described previously in connection with FIG. 4.

Further, the embodiment of FIG. 6 corresonding to the FIG. 3 photoelectric conversion device of the present invention is identical in construction with the embodiment of FIGS. 1 to 3 except that the isolating portion H_(j) consists of the groove 16 defined between the electrodes F_(j) and F_(j+1) and the oxide 17 of the non-single-crystal semiconductor forming the non-single-crystal semiconductor laminate member Q_(j), which is formed in the upper half portion thereof.

Such isolating portions H_(j) can easily be formed by carrying out in an oxygen atmosphere the laser beam scanning of the conductive layer 43 described previously with respect to FIG. 5.

Likewise, the embodiment of FIG. 7 is identical in construction with the embodiment of FIGS. 1 to 3 except that the isolating portion H_(j) is formed by an oxide 18 which results from oxidation of the conductive material forming the electrodes F_(j) and F_(j+1) and separates them as shown. Such isolating portions H_(j) can easily be formed by the same laser beam scanning as that employed for the embodiment of FIG. 6.

The embodiment of FIG. 8 is also identical in construction with the embodiment of FIGS. 1 to 3 except that the isolating portion H_(j) is formed by the groove 16 which barely extends into the non-single-crystal semiconductor laminate member Q_(j) but separates the electrodes E_(j) and E_(j+1) as shown. Such isolating portion H_(j) can easily be formed by adjusting the scanning speed and/or power of the laser beam in the laser beam scanning as in the embodiment of FIG. 4.

It is evident that all the arrangements of the embodiments having the isolating portions H_(j), shown in FIGS. 5 to 8, have the same features as those of the embodiment of FIGS. 1 to 3, though not described in detail.

In the embodiment of FIGS. 1 to 3, the groove O_(j), which separates the non-single-crystal semiconductor laminate member Q_(j) and Q_(j+1) of the semiconductor elements U_(j) and U_(j+1) and through which extends the coupling portion K_(j) for connecting the electrode F_(j+1) of the semiconductor element U_(j+1) to the electrode E_(j) of the semiconductor element U_(j), is provided on the side of the electrode E_(j) at a position a predetermined distance apart from the groove G_(j) which defines the semiconductor elements U_(j) and U_(j+1).

The embodiment of FIG. 9 corresponding to FIG. 3 is identical in construction with the embodiment of FIGS. 1 to 3 except that the grooves O_(j) and G_(j) intercommunicate in the lateral direction and, consequently, the electrode E_(i) has no portion 14.

The embodiment of FIG. 9, though not described in detail, has the same features as those of the embodiment of FIGS. 1 to 3.

In addition, since the electrode E_(i) has no portion 14, the photovoltage of the semiconductor element U_(i) can be increased correspondingly with the same area of the substrate 1 occupied by the electrode E_(i) as compared with the photovoltage obtainable with the embodiment of FIGS. 1 to 3, or the same photovoltage can be obtained with the smaller length of the electrode E_(i) in the lateral direction than in the first embodiment.

Accordingly, the embodiment of FIG. 9 is smaller in size but larger in electromotive force than the embodiment of FIGS. 1 to 3.

The embodiment of FIG. 10 is also identical in construction with the embodiment of FIGS. 1 to 3 except that as is the case with the embodiment of FIG. 9, the grooves O_(j) and G_(j) interconnect in the lateral direction and, accordingly, the electrode E_(j) has no portion 14. In the embodiment of FIG. 10, however, half of the groove O_(j) on the opposite side from the groove G_(j) does not extend entirely across the electrode E_(j) in its thickwise direction. In the case where the electrodes E_(j) and E_(n) are each comprised of the reflective conductive layer 4 and the light transparent conductive layer 5, since their materials are different, the abovesaid groove O_(j) can easily be formed by the laser beam scanning of the non-single-crystal semiconductor laminate member 42 and the electrodes E₁ to E_(n) described previously with respect to FIG. 4.

The embodiment of FIG. 10 also possesses the same advantages as does the embodiment of FIG. 9.

In the embodiment of the photoelectric conversion device of the present invention depicted in FIGS. 1 to 3, the groove O_(j) extends through the electrode E_(j) to reach the substrate 1, and the coupling portion K_(j) makes contact only with the side of the electrode E_(j) exposed to the groove O_(j).

In another embodiment of the photoelectric conversion device of the present invention, however, as shown in FIG. 11, the groove O_(j) is not completely through the electrode E_(j) but is through only layer 5 of the electrode E_(j) and the coupling portion K_(j) is formed to make contact with the layer 4 of the electrode E_(j) exposed to the groove O_(j).

In another embodiment of the photoelectric conversion device of the present invention, however, as shown in FIG. 12, the groove O_(j) is not extended into the electrode E_(j) at all and the coupling portion K_(j) is formed to make contact only with the top of the electrode E_(j) exposed to the groove O_(j).

In the embodiments illustrated in FIGS. 11 and 12, the groove O_(j) can easily be formed by the same laser beam scanning as that for the non-single-crystal semiconductor laminate member Q_(j) described previously with respect to FIG. 4 but, in this case, the intensity of the laser beam is adjusted suitably.

It will be seen that any of the structures of the embodiments provided with the grooves shown in FIGS. 11 and 12 possesses the same advantages as are obtainable with the embodiment of FIGS. 5 to 11, though not described in detail.

In the embodiment of FIGS. 1 to 3, the series connected array of the semiconductor elements U₁ to U_(n) constituting one photoelectric conversion device on the substrate 1 is connected at one end to the external connection terminal 11, which is formed by the extended portion of the electrode E₁ of the semiconductor element U₁ on the substrate 1, and connected at the other end to the external connection terminal 12 which is formed by the extended portion of the electrode F₀ on the substrate 1 and connected to the electrode E_(n) through the coupling portion K_(n).

In another embodiment of the present invention, however, a plurality a×b of such photoelectric conversion devices, each made up of the n semiconductor elements U₁ to U_(n) connected in series as shown in FIGS. 1 and 2, are arranged in the form of a matrix consisting of a rows and b columns as illustrated in FIGS. 13 and 14 corresponding to FIGS. 1 and 2. In FIGS. 13 and 14 reference character M_(rs) (r=1, 2, . . . a and s=1, 2, . . . b) indicates each photoelectric conversion device disposed at one of the intersections of rows and columns. The photoelectric conversion devices M₁₁ to M_(1b), M₂₁ to M_(2b), . . . and M_(a1) to M_(ab) are isolated by grooves 26 from adjacent ones of them.

In the embodiment illustrated in FIGS. 13 and 14, the photoelectric conversion device M_(rs) is identical in construction with the photoelectric conversion device of the embodiment of FIGS. 1 to 3 except in the following points:

An electrode E₀ similar to the electrodes E₁ to E_(n) is formed on the substrate 1 on the side of the electrode E₁ of the semiconductor element U₁ on the opposite side from the electrode E₁ and the electrode E₀ is isolated by a groove G₀ similar to G₁ to G_(n-1).

Further, the non-single-crystal semiconductor laminate member Q₁ of the semiconductor element U₁ does not extend from the electrode E₁ to the substrate surface but instead it extends across the groove G₀ to the marginal edge of the electrode E₀.

The electrode F₁ of the semiconductor element U₁, which is formed to cover the non-single-crystal semiconductor laminate member Q₁ and extend to the substrate 1 in the first embodiment, is formed to extend to the marginal edge of the non-single-crystal semiconductor laminate member Q₁ correspondingly. And the external connection terminal 11 is formed by the end portion of the electrode F₁ on the non-single-crystal semiconductor laminate member Q₁ on the opposite side from the electrode F₂.

Moreover, as shown in FIG. 11, the non-single-crystal semiconductor laminate member Q_(n) of the semiconductor element U_(n) is formed to extend to the marginal edge of the electrode E_(n).

The electrode F₀, though formed to cover the non-single-crystal semiconductor laminate member Q_(n) and to extend to the substrate 1 in the embodiment of FIGS. 1 to 3, extends to the marginal edge of the non-single-crystal semiconductor laminate member Q_(n) correspondingly. And the external connection terminal 12 is formed by the end portion of the electrode F₀ on the non-single-crystal semiconductor laminate member Q_(n) on the opposite side from the electrode F_(n).

The above is a description of the abovesaid another embodiment of the photoelectric conversion device of the present invention.

The photoelectric conversion device of such a construction can be obtained by a manufacturing method similar to that employed for the fabrication of the photoelectric conversion device of the embodiment of FIGS. 1 to 3.

That is, as shown in FIGS. 15A to 15G corresponding to FIGS. 4A to 4G, a×b photoelectric conversion devices M₁₁ to M_(1b), M₂₁ to M_(2b), . . . and M_(a1) to M_(ab) are formed on the substrate 1 by a sequence of steps similar to those shown in FIGS. 4A to 4G, though not described in detail.

Next, as shown in FIG. 15H, the grooves 26 are formed by the same laser beam scanning as described previously with respect to FIG. 4.

Next, the light transparent antireflection and protective film 15 (not shown) is formed.

In this way, the structure of the embodiment referred to previously in conjunction with FIGS. 13 and 14 is obtained.

The above is a description of the abovesaid another embodiment and its manufacturing method.

The photoelectric conversion device of FIGS. 13 and 14 is identical in construction with the embodiment of FIGS. 1 to 3 except in the abovesaid points, and hence presents the same advantages as those obtainable with the embodiment of FIGS. 1 to 3, though not described in detail.

Moreover, according to the embodiment of FIGS. 13 and 14, the photoelectric conversion devices M₁₁ to M_(1b), M₂₁ to M_(2b), . . . and M_(a1) to M_(ab) are formed on the substrate 1 and separated by the grooves 26 and the substrate 1 is formed by the insulating sheet-like member, so that it can easily be severed at the positions of the grooves 26 into a×b independent photoelectric conversion devices.

Incidentally, the embodiment of FIGS. 13 and 14 can also be modified and varied in the same manner as in the embodiments of FIGS. 5 to 12 which are modifications and variations of the embodiment of FIGS. 1 to 3.

It will be apparent that may modifications and variations may be effected without departing from the scope of the novel concepts of the present invention. 

What is claimed is:
 1. A method of making a photoelectric conversion device, comprising the steps of:preparing a substrate formed by an insulating sheet-like member having a metallic sheet-like member and an insulating film having a thermal conductivity less than that of glass formed on the metallic sheet-like member; forming a first conductive layer on the insulating film of the substrate; forming n-1 (where n is an integer larger than 2) sequentially arranged first grooves G₁ to G_(n-1) in the first conductive layer by using a first laser beam to form n sequentially arranged first electrodes E₁ to E_(n) separated by the first grooves G₁ to G_(n-1), respectively; forming on the substrate a non-single-crystal semiconductor laminate layer having formed therein at least one semiconductor junction to cover the first grooves G₁ to G_(n-1) and the first electrodes E₁ to E_(n) ; forming n-1 sequentially arranged second grooves O₁ to O_(n-1) in the non-single-crystal semiconductor laminate layer by using a second laser beam to form n sequentially arranged non-single-crystal semiconductor laminate members Q₁ to Q_(n) defined by the second grooves O₁ to O_(n-1), respectively, thereby to expose portions of the respective first electrodes E₁ to E_(n-1) to the outside, where the grooves O₁ to O_(n-1) do not extend to the metallic sheet-like member of the substrate due to the low thermal conductivity of the insulating film; forming a second conductive layer which continuously extends on the non-single-crystal semiconductor laminate members Q₁ to Q_(n) and extends into the grooves O₁ to O_(n-1) to provide coupling portions K₁ to K_(n-1) which are connected to the first electrodes E₁ to E_(n-1) through the grooves O₁ to O_(n-1), respectively, and; forming n-1 sequentially arranged isolating portions H₁ to H_(n-1) in the second conductive layer on the non-single-crystal semiconductor laminate members Q₁ to Q_(n-1), respectively, to form n sequentially arranged second electrodes F₁ to F_(n) which are isolated by the isolating portions H₁ to H_(n-1), respectively, and opposite the first electrodes E₁ to E_(n) through the non-single-crystal semiconductor laminate members Q₁ to Q_(n), respectively, the second electrode F_(j+1) (j=1, 2, 3, . . . (n-1) being connected to the first electrode E_(j) through the coupling portion K_(j).
 2. A method of making a photoelectric conversion device according to claim 1, wherein the formation of the grooves G₁ to G_(n-1) is carried out in the air.
 3. A method of making a photoelectric conversion device according to claim 1, wherein the formation of the groove G₁ to G_(n-1) is carried out in an atmosphere of a gas or a liquid which reacts with the material of the first conductive layer at high temperature to spatter it from the surface of the substrate.
 4. A method of making a photoelectric conversion device according to claim 3, wherein the gas is hydrogen fluoride, hydrogen chloride, or a Freon gas, and wherein the liquid is hydrofluoric acid, hydrochloric acid, or a Freon liquid.
 5. A method of making a photoelectric conversion device according to claim 1, wherein the second groove O_(j) (j=1, 2, . . . (n-1)) is formed a predetermined distance apart from the first groove G_(j) but adjacent thereto, and wherein the isolating portion H_(j) is formed a predetermined distance apart from the first groove G_(j) and the second groove O_(j) and adjacent to the second groove O_(j).
 6. A method of making a photoelectric conversion device according to claim 1, wherein the second groove O_(j) (j=1, 2, . . . (n-1)) is formed to extend through the first electrode E_(j) so that the coupling portion K_(j) may be connected with the side of the first electrode E_(j) which is exposed by the second groove O_(j).
 7. A method of making a photoelectric conversion device according to claim 1, wherein the formation of the grooves O₁ to O_(n-1) is carried out in the air.
 8. A method of making a photoelectric conversion device according to claim 1, wherein the formation of the grooves O₁ to O_(n-1) is carried out in an atmosphere of a gas or a liquid which reacts with the material of the non-single-crystal semiconductor laminate member at high temperature to spatter it from the surface of the substrate.
 9. A method of making a photoelectric conversion device according to claim 8, wherein the gas is hydrogen fluoride, hydrogen chloride, or a Freon gas, and wherein the liquid is hydrofluoric acid, hydrochloric acid, or a Freon liquid.
 10. A method of making a photoelectric conversion device according to claim 1, wherein the formation of the isolating portions H₁ to H_(n-1) is carried out in the air.
 11. A method of making a photoelectric conversion device according to claim 1, wherein the formation of the isolating H₁ to H_(n-1) is carried out in an atmosphere of a gas or a liquid which reacts with the material of the second conductive layer at high temperature to spatter it from the surface of the substrate.
 12. A method of making a photoelectric conversion device according to claim 11, wherein the gas is hydrogen fluoride, hydrogen chloride, or a Freon gas, and wherein the liquid is hydrofluoric acid, hydrochloric acid, or a Freon liquid.
 13. A method of making a photoelectric conversion device according to claim 1, wherein the formation of the isolating portions H₁ to H_(n-1) is carried out in an atmosphere of oxygen.
 14. A method of making a photoelectric conversion device according to claim 1, wherein the formation of the isolating portions H₁ to H_(n-1) is carried out so that the isolating portion H_(j) may extend into the non-single-crystal semiconductor laminate member Q_(j).
 15. A method of making a photoelectric conversion device according to claim 1 where the thickness of said insulating film is 0.1 to 5 um.
 16. A method of making a photoelectric conversion device according to claim 1 wherein said insulating film comprises an organic resinous material having a melting point less than that of glass.
 17. A method of making a photoelectric conversion device according to claim 16 where said organic resinous material is selected from the group consisting of polyethylene terephthalate resins, polyimide resins, polyether sulfone resins, and polyether ketone resins.
 18. A method of making a photoelectric conversion device according to claim 17 where said organic resinous material is a polyimide resin. 